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SENSORLESS FIELD ORIENTED CONTROL OF BRUSHLESS ...

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Figure 2.20 – Elementary brushless PM motors with concentrated full-pitch winding.<br />

The rotor magnets produce airgap flux densities as shown in Figure 2.21. The motor on the left<br />

has magnets that produce an airgap flux density that is a sinusoidal function of the angle around<br />

the rotor, α. The motor on the right has magnets that produce an airgap flux density that is also a<br />

function of the angle around the rotor but whose shape is difficult to describe. However, it has the<br />

notable feature that the magnitude is constant over an angular pitch of β≥120°; note that β has<br />

correspondence between Figure 2.20 and Figure 2.21. If these segments are centered about α=0°<br />

and α=180°, the airgap flux density could be approximated by the trapezoid shown in dashed<br />

lines. These two elementary models are representative of the two most common types of non-<br />

salient BPMS motors (real motors are not always constructed as shown). The motor on the left is<br />

a sinusoidal motor and the motor on the right is an arbitrary trapezoidal motor.<br />

Figure 2.21 – Airgap flux density profiles for two BPMS motors.<br />

The airgap flux densities shown in Figure 2.21 are defined in terms of the angle α around the<br />

rotor. But since the coilsides that compose the winding have fixed positions it is possible to<br />

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